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SOLID STATE PHYSICS (3C25) Solutions to problem paper 1 1 ...

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(f) Why is this surprising? [2]<br />

The body centred cubic crystal has a cubic cell for which h=1. However<br />

the basis introduces extra planes.<br />

3. When electrons are scattered from a crystal surface<br />

(a) Why does the angle of incidence equal the angle of reflection? [2]<br />

To ensure that the waves scattered off neighbouring surface a<strong>to</strong>ms are<br />

in phase.<br />

(b) Why do you only see reflections at some angles of incidence? [2]<br />

Because only for certain angles of incidence are the waves scattered off<br />

neighbouring planes in phase.<br />

(c) Why can you study only a<strong>to</strong>ms near the crystal surface? [2]<br />

Electrons cannot penetrate deep in<strong>to</strong> a crystal because they are scattered<br />

by the surface layers of a<strong>to</strong>ms.<br />

4. Consider the scattering of x-rays of wavelength λ from a face centred cubic<br />

crystal with cubic lattice constant a.<br />

(a) What are the allowed scattering angles when the scattering is from the<br />

(001) planes of the crystal? (Use Bragg’s law.) [3]<br />

2d sin θ = nλ<br />

d = a/2<br />

⇒ sin θ = nλ<br />

a<br />

(b) Using the simple cubic representation of a face centred cubic crystal,<br />

write down the primitive translation vec<strong>to</strong>rs and calculate the reciprocal<br />

lattice vec<strong>to</strong>rs. [3]<br />

a = a(100) A = 2π<br />

a (100)<br />

b = a(010) B = 2π<br />

a (010)<br />

c = a(001) C = 2π<br />

a (001)<br />

(c) Using the Laue construction, determine the allowed scattering vec<strong>to</strong>rs for<br />

scattering from (001) planes. [4]<br />

In general, a reflection from a (001) surface implies that ∆ k is parallel<br />

<strong>to</strong> C (the primitive reciprocal lattice vec<strong>to</strong>r with indices (001)). From the<br />

Laue construction we know that scattering vec<strong>to</strong>rs must equal reciprocal<br />

lattice vec<strong>to</strong>rs for strong reflection:<br />

2

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